INGENIA

AST-03

Bondi accretion

Ṁ = 4π λ ρ (G M)² / c_s³. Spherical accretion onto a point mass.

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GravityBondi

Governing equation

M˙=4πλρ(GM)2/cs3\dot M=4\pi\lambda\rho (GM)^2/c_s^3

where

M
Mass (M_\odot)
\rho
Density (10⁻²⁰ kg/m³)
c_s
Sound speed (km/s)
\lambda
Bondi λ ()
\dot M
Accretion rate (M_\odot/yr)

Lecture brief

Historical brief

Hubble expansion, Jeans collapse, Eddington luminosity, Bondi accretion and Stefan–Boltzmann stars are the first astrophysical budgets. The sheets scale a star, a cloud and a horizon. This sheet (AST-03 — Bondi accretion) is the form associated with Bondi. Working symbols: MM, ρ\rho, csc_s, λ\lambda \rightarrow M˙\dot M. λ ~ 1 for γ = 5/3. The Bondi radius is G M / c_s².

Purpose

Purpose: compute M˙\dot M from MM, ρ\rho, csc_s, λ\lambda in Astrophysics via M˙=4πλρ(GM)2/cs3\dot M=4\pi\lambda\rho (GM)^2/c_s^3 Ṁ = 4π λ ρ (G M)² / c_s³. Spherical accretion onto a point mass. Use it when a real astrophysics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given M=10.000ModotM = 10.000\,\mathrm{M_odot}, \rho = 1.000\,\mathrm{10⁻^{2}⁰ kg/m^{3}}, cs=10.000km/sc_s = 10.000\,\mathrm{km/s}, λ=1.000\lambda = 1.000\,\mathrm{—}, the governing relation M˙=4πλρ(GM)2/cs3\dot M=4\pi\lambda\rho (GM)^2/c_s^3 yields M˙=3.513e12Modot/yr\dot M = 3.513e-12\,\mathrm{M_odot/yr}. A star, an inward spherical flow. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Accretion rate \dot M0.0000 M_\odot/yr
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AST-03 · star
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Narration of this film

A star, an inward spherical flow.

λ ~ 1 for γ = 5/3. The Bondi radius is G M / c_s².

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